Term
|
Definition
|
|
Term
|
Definition
|
|
Term
|
Definition
power per unit area received by an observer
I ∝ A
(Wm-2)
|
|
|
Term
|
Definition
| link parts of a wave that are in phase |
|
|
Term
|
Definition
| direction of energy flow (at 90⁰ to wavefront) |
|
|
Term
|
Definition
represents the motion (oscillation) at one point on the wave
every point will oscillate in the same manner but start their oscillation at different times |
|
|
Term
| displacement-position graph |
|
Definition
represents a 'snapshot' of a wave
over time it will move on but keep the same shape |
|
|
Term
|
Definition
transverse waves
travel at the speed of light (3 x 10^8)
gamma<Xrays<UV<Visible<IR<Microwave<TV<Radio
(in terms of wavelength) |
|
|
Term
|
Definition
| shortest distance between two points along a wave that are in phase |
|
|
Term
| when waves move between two media |
|
Definition
there will be both reflection and transmission at the boundary
|
|
|
Term
| method of drawing waefronts to show reflection |
|
Definition
1. draw normal
2. draw reflected ray
3. draw wavefronts at 90⁰ to ray |
|
|
Term
| does frequency change when a wave is refracted? |
|
Definition
|
|
Term
| when slowing down the wave moves ______ the normal |
|
Definition
|
|
Term
when speeding up the wave moves ______ the normal
|
|
Definition
|
|
Term
| the bigger value of n .... |
|
Definition
| the slwer the wave is travelling |
|
|
Term
| method of drawing waefronts to show refraction |
|
Definition
1. draw normal
2. draw refracted ray
3. draw wavefronts at 90 degrees to ray |
|
|
Term
| the closer the size of the gap to the wavelength of the wave.... |
|
Definition
| the greater the diffraction |
|
|
Term
| longer wavelengths will diffract _____ than shorter wavelengths |
|
Definition
|
|
Term
| effect of sound waves having a larger wavelength than light |
|
Definition
| sound diffracts more around corners |
|
|
Term
| are long wavelength radio stations received better in hilly areas or are short wavelength radio stations received better? |
|
Definition
| long wavelength radio stations are received better |
|
|
Term
| when two in phase waves meet.... |
|
Definition
| constructive interference occurs |
|
|
Term
| when two out of phase (by 90degrees) waves meet ... |
|
Definition
|
|
Term
| path difference for nodal lines |
|
Definition
destructive interference
(n + 0.5) x wavelength |
|
|
Term
| path difference for antinodal lines |
|
Definition
constructive interference
n x wavelength |
|
|
Term
|
Definition
fired alpha particles at thin gold foil, with a fluorescent screen to detect where they went
- gold is very thin (1000 atoms) and is a large atom
- helium nuclei as it is positively charged and small mass |
|
|
Term
| Observations and conclusions of Rutherford Experiment |
|
Definition
- most of alpha particles passed through the foil unaffected as most of an atom is empty space
- a significant number of alpha particles had their path deflected as they passed through the foil as the positive charge of an atom is concentrated in the centre and the electrons orbit this nucleus
- some alpha particles bounced straight back from the gold foil as most of the mass of an atom is in the nucleus |
|
|
Term
| evidence of atomic energy levels |
|
Definition
emission and absorption spectra
an electron can move between energy levels by either absorbing or emitting a photon |
|
|
Term
|
Definition
only photons of specific wavengths (and frequency) emitted
white bands on dark |
|
|
Term
|
Definition
only photons of specific wavelengths (and frequencies) absorbed
set-up by passing light through cold gas (gas absorbs certain wavelengths are leaves remaining colours to be passed onto screen) |
|
|
Term
| protons and neutrons held together in nucleus |
|
Definition
strong nuclear force which is balanced by the repulsion between the protons (Coulomb interaction) and is short range and involves neutrons in some way
(larger nuclei have proportionally more neutrons) |
|
|
Term
|
Definition
| need the 'right' combination of protons and neutrons, otherwise decay to form smaller nuclei (radioactivity) |
|
|
Term
|
Definition
each form is known as a nuclide
different number of neutrons but same number of protons |
|
|
Term
|
Definition
- helium nucleus
- about 5cm range
- stopped by paper
- very high ionising ability (high Ek, positive charge and relatively large mass) |
|
|
Term
|
Definition
- beta -ve is an electron emitted from the nucleus (neutron--> proton)
- beta +ve is a positive electron or positron emitted from the nucleus (proton --> neutron)
- about 30cm range
- stopped by aluminium
- low ionising ability
- beta -ve particles are accompanied by antineutrinos
- beta +ve particles are accompanied by neutrinos (v) |
|
|
Term
|
Definition
- electronmagnetic radiation (photons)
- range of hundreds of metres (high energy)
- stopped by thick lead
- very low ionising ability
- always accompanies alpha and beta radiation |
|
|
Term
|
Definition
| a region of space where a charged object experiences a force due to its charge |
|
|
Term
| direction of electric field |
|
Definition
| the direction shows the force that would act on a positive test charge placed at that point |
|
|
Term
| direction of electric field lines for a positive charge ___ |
|
Definition
|
|
Term
|
Definition
| the force between two point charges is proportional to the product of their charges and inversely proportional to the square of their separation |
|
|
Term
|
Definition
| the force per unit charge experienced by a small positive test charge placed in the field (a test charge is a charge that does not affect the electric field) |
|
|
Term
| Newton's universal law of gravitation |
|
Definition
| every single point mass attracts every other point mass with a force that is directly proportional to the product of their masses and inversely proportional to the square of their separation |
|
|
Term
| Masses in a gravitational field |
|
Definition
| both masses wil experience the same size force but the effect of the force will depend on the masses involved |
|
|
Term
|
Definition
| a region of space where a mass experiences a force because of its mass |
|
|
Term
| gravitational field strength |
|
Definition
| the force per unit mass experienced by a small test mass placed in the field |
|
|
Term
| field strength at a point between two masses |
|
Definition
sum of the two individual field strengths
(found through vector equations) |
|
|
Term
| derivation of formula for the gravitational field strength at the surface of a planet |
|
Definition
g = F/m
F = (GMm)/(r^2)
g = ((GMm)/(r^2))/m
g = (GM)/(r^2) |
|
|
Term
| similarities between gravitational field and electric field |
|
Definition
forces can act at a difference (don't have to be in contact)
force is inversely proportional to r^2
|
|
|
Term
| differences between gravitational field and electric field |
|
Definition
- gravitational field always attract, but electric field can attract or repel depending on charge
- gravitational field depends on mass, and electric field depends on charge
- field lines show force on any mass for gravitational field, and show force on positive charge for electric field |
|
|
Term
|
Definition
- positive charges
- thumb is motion
- palm is force
- fingers are direction of field |
|
|
Term
| force us always at right abgles to the velocity of the charge |
|
Definition
| resultant motion is circular |
|
|
Term
|
Definition
|
|
Term
|
Definition
- thumb is current direction
- fingers are field direction |
|
|
Term
| SHM takes place when the acceleration of (and force on) an object is: |
|
Definition
- proportional to its displacement from its equilibrium position
- directed towards its equilibrium position (restoring force) |
|
|
Term
| maximum and minium force acting in SHM |
|
Definition
max occurs at -Xo and +Xo
min occurs at 0 |
|
|
Term
| defining equation for SHM |
|
Definition
|
|
Term
|
Definition
| damping involves a force that is always in the opposite direction to the direction of motion of the oscillating particle (it dissipates SHM) |
|
|
Term
|
Definition
- car suspension
- electric meters with moving pointers (critical)
- some door closing mechanisms (critical) |
|
|
Term
| the amplitude of the oscillation decreases when damped but the _____ does not change |
|
Definition
|
|
Term
|
Definition
| occurs when a system is forced to oscillate at its natural frequency (large amplitude) |
|
|
Term
| Examples of good resonance |
|
Definition
- microwaves (water resonates)
- radio receivers
- musical instruments
- quartz crystals (clocks) |
|
|
Term
| Examples of bad resonance |
|
Definition
- poorly designed buildings in earthquakes
- vibrations in machines |
|
|
Term
|
Definition
|
|
Term
low energy --> high energy
(low frequency --> high frequency) |
|
Definition
| Radio<IR<ROYGBIV<UV<XRays |
|
|
Term
| below a certain threshold frequency of incident light... |
|
Definition
| no electrons are emitted (each metal has its own specific threshold frequency) because it is the energy needed to release electrons |
|
|
Term
| the maximum kinetic energy of an electron is dependent on... |
|
Definition
| the frequency of the incident light |
|
|
Term
| effect of increasing intensity of incident light |
|
Definition
| more electrons are emittend but the energy of the electrons does not change |
|
|
Term
| lower work function means... |
|
Definition
| less energy is required (easier for electrons to escape) and lower threshold frequency |
|
|
Term
|
Definition
| the minimum amount of energy required by the electrons on the surface of the metal to escape |
|
|
Term
| the amount of energy carried by a photon depends on... |
|
Definition
| the frequency of the light |
|
|
Term
| the higher the intensity the ____ photons arrive per second |
|
Definition
"more"
energy level does not increase
one electron per photon (when one photon arrives one electron can leave if there is enough energy in photon) |
|
|
Term
| energy of photon greater than or equal to work function |
|
Definition
| electron is emitted, and any excess energy is given to the electron as kinetic energy |
|
|
Term
| energy of photon < work function |
|
Definition
| energy is shared between electrons and none are emitted |
|
|
Term
|
Definition
| 238U --> 234Th + 4He + energy |
|
|
Term
|
Definition
| 14C --> 14N + B- + antineutrino + energy |
|
|
Term
|
Definition
| spontaneous and random(don't know which particular nucleus will decay) |
|
|
Term
|
Definition
| the time taken for the activity to fall to 50% of the initial value |
|
|
Term
|
Definition
large nuclei broken into smaller nuclei
(two atoms + neutrons + energy)
|
|
|
Term
|
Definition
small nuclei combined if pressure and temperature high enough
(neutron and energy also emitted) |
|
|
Term
| release of energy during fission/fusion |
|
Definition
| different nuclei are at different energy levels, if the products of a nuclear reaction are at a lower energy state than the reactants energy is released |
|
|
Term
|
Definition
the amount of energy required to hold a nucleus together
(the amount needed to break it apart) |
|
|
Term
| binding energy per nucleon |
|
Definition
| (total binding energy of the nucleus)/(number of nucleons) |
|
|
Term
| the greater the binding energy per nucleon... |
|
Definition
| the more stable the nucleus (the more energy is needed to break it apart) |
|
|
Term
|
Definition
|
|
Term
|
Definition
|
|
Term
|
Definition
|
|
Term
| derive the formula for half life with respect to ln and λ |
|
Definition
N = Noe- λt
No/2 = Noe- λt/2
0.5 = e- λt/2
ln(0.5) = - λT0.5
T(half life) = (ln2)/λ
|
|
|
Term
| Each line on the emission spectrum for a particular element corresponds to ... |
|
Definition
| a photon that is emitted by an electron within an atom of the element |
|
|
Term
|
Definition
| the electrons are at a higher than normal energy level due to the element being heated up (hot gas). As an electron falls to a lower energy level it will emit a photon of a frequency that corresponds to the energy difference between the 2 levels |
|
|
Term
|
Definition
| wave-particle duality of light |
|
|
Term
| method to find the de Broglie wavelength of an electron |
|
Definition
1. find the speed of the electron using
Ve = 0.5 x m x v2
2. find the wavelength using de Broglie formula (p=h/f) |
|
|
Term
|
Definition
- confirmed the de Broglie hypothesis
- accelerated electrons at a diffraction grating
- experiment showed intereference pattern of electrons
- dimensions of interference pattern matched the expected wavelength of the accelearate electrons
- the distance between the 'antinodes' is that expected by the wavelength of the electron |
|
|
Term
|
Definition
the total amount of energy emitted by a star per second
(unit: W) |
|
|
Term
|
Definition
|
|
Term
|
Definition
how bright stars appear to an observer
(the amount of energy received per second per unit area)
unit: Wm-2 |
|
|
Term
| determining composition of stars |
|
Definition
analysing the spectra of light emitted
the elements in the star will absorb light leaving dark lines in the spectra
|
|
|
Term
|
Definition
radiation pressure = gravitational pressure
(outwards) (inwards) |
|
|
Term
|
Definition
a group of stars held together by gravity
each star is relatively close to each other |
|
|
Term
|
Definition
| a group of stars in a region of the sky that appear to make a pattern. The stars may be relatively far from each other |
|
|
Term
|
Definition
| A region with a large number of stars plus gas and dirt helf together by fravity |
|
|
Term
|
Definition
|
|
Term
|
Definition
|
|
Term
|
Definition
theoretical object that is a perfect emitter (and absorber) of radiation
(emit a continuous spectrum of radiation) |
|
|
Term
| peak wavelength of black body |
|
Definition
dependent on temperature of object
as temperature increases, the peak wavelength gets shorter and the frequency increases |
|
|
Term
|
Definition
O - blue B - blue/white A - white F - yellow/white G - yellow K - orange M - red
(decreasing in temperature to M) |
|
|
Term
|
Definition
| unstable, vary in brightness and size, rare |
|
|
Term
|
Definition
| big, red (low temperature) late stage in life cycle, fusion of elements other than H (reason why cool) |
|
|
Term
|
Definition
| small, white (hot) smaller than sun, final stage for some stars, fusion finished now cooling--> brown dwarf |
|
|
Term
|
Definition
magnitude 1 = brightest
magnitude 6 = just visible to naked eye |
|
|
Term
|
Definition
| dependent on distance from Earth and luminosity |
|
|
Term
|
Definition
|
|
Term
| methods used to measure distance to stars |
|
Definition
1. parallax
2. spectroscopic parallax
3. cepheid variable |
|
|
Term
|
Definition
| the apparent shifting of an object against a distance background when viewed from 2 different perspectives |
|
|
Term
|
Definition
1. can measure up to 100pc using telescopes on Earth
2. above this the able p is too small and is within the uncertainty of the measurement |
|
|
Term
| Spectroscopic parallax steps (5) |
|
Definition
1. Observe the spectrum of the star
2. Find the peak wavelength of the light emitted
3. Calculate the temperature of the star using Wein's Law
(max wavelength = (2.90 x 10-3)/T
4. Using the HR diagram to find luminosity of the star (if it is a main sequence star)
5. Measure the apparent brightness from Earth and then calculate the star's distance away
(b = L/(4pid2) |
|
|
Term
| Limitation of spectroscopic parallax |
|
Definition
can only be used for distances up to 10Mpc
(beyond that there is too much error when observing the spectrum) |
|
|
Term
|
Definition
used for distances greater than 10Mpc
1. Find the period by observation
2. Get the luminosity from the period-luminosity graph
3. Measure apparent brightness on Earth
4. Use b=L/(4pid2) to calculate the distance |
|
|
Term
| Newton's model of the universe |
|
Definition
- uniform
- static
- infinite (in space and time) |
|
|
Term
|
Definition
1. based on the reality that the night sky is dark (not bright)
2. if a shell has a thickness (t) and a number of stars per unit volume (n)
No. of stars in shell = area of shell x t x n
= 4πr2 x t x n
3. number of stars is proportional to r2, and the apparent brightness is proportional to 1/r2
4. no matter the distance the stars would be equally bright and cause the sky to be infinitely bright
IT IS DARK AT NIGHT... |
|
|
Term
| Today's model of the universe |
|
Definition
1. created 15 billion years ago (Big Bang)
2. All the matter in today's universe was contained in a single very hot, very dense point --> singularity
4. This rapidly expanded (and cooled) creating space and time
the universe is NOT expanding into space, but creating it |
|
|
Term
| Evidence for today's model of the universe |
|
Definition
1. Light from galaxies is red-shifted showing they are all moving away from each other --> the universe is expanding
2. Penzias and Wilson (1960s) discovered microwave radiation coming from all directions in space. The wavelength suggests that it is being emitted by an object that has a temperature of 3K (temperature of universe after 15 billion years of cooling) |
|
|
Term
| Outcomes for the Universe |
|
Definition
1. Open Universe (gravity is not strong enough to stop expansion, but gravity slows it dowm)
2. Flat (gravity slows expansion but takes an infinite period of time to stop - if it stopped then gravity would cause it to collapse)
3. Closed (gravity causes the universe to collapse back in on itself) |
|
|
Term
| Outcome of universe depends on... |
|
Definition
the density of the universe
1. open: p>po
2. flat: po
closed: p<po |
|
|
Term
|
Definition
|
|
Term
|
Definition
Massive
Astronomical
Compact
Halo
Objects
e.g. high mass planets, 'failed' stars, blackholes
|
|
|
Term
|
Definition
Weakly
Interacting
Massive
Particles
e.g. hypothetical particles |
|
|